Are the Positive-Parity Mesons in the 405 Multiplet?
M. Resnikoff, Richard R. Silbar
Abstract
M. Resnikoff, Richard R. Silbar
Abstract
The 405 multiplet mass formulas, derived previously, are used to predict the masses of the positive-parity mesons. Using three ${2}^{+}$ mesons (${f}_{0}$, ${A}_{2}$, ${K}^{**}$) as input, the ${f}^{\ensuremath{'}}$ is predicted in agreement with experiment, and the states of the ${2}^{+}$27-plet are found to lie higher, but in the accessible experimental region. The existence of the 27-plet states is a clear test of whether the 405 multiplet exists. When the ${1}^{+}$ mesons $D(1286)$ and $E(1420)$ are taken together with the three ${2}^{+}$ mesons as input, the remaining $J={0}^{+}, {1}^{+}$ mesons are predicted. Mass-difference equalities are presented and comparison is made with experiment.
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The 405 multiplet mass formulas, derived previously, are used to predict the masses of the positive-parity mesons. Using three ${2}^{+}$ mesons (${f}_{0}$, ${A}_{2}$, ${K}^{**}$) as input, the ${f}^{\ensuremath{'}}$ is predicted in agreement with experiment, and the states of the ${2}^{+}$27-plet are found to lie higher, but in the accessible experimental region. The existence of the 27-plet states is a clear test of whether the 405 multiplet exists. When the ${1}^{+}$ mesons $D(1286)$ and $E(1420)$ are taken together with the three ${2}^{+}$ mesons as input, the remaining $J={0}^{+}, {1}^{+}$ mesons are predicted. Mass-difference equalities are presented and comparison is made with experiment.
Key concepts: Multiplet, Meson, Physics, Parity (physics), Particle physics, Nuclear physics, Quantum mechanics, Spectral line